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US20090103305A1 - High-pressure gas discharge lamp - Google Patents

High-pressure gas discharge lamp Download PDF

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Publication number
US20090103305A1
US20090103305A1 US10/596,808 US59680804A US2009103305A1 US 20090103305 A1 US20090103305 A1 US 20090103305A1 US 59680804 A US59680804 A US 59680804A US 2009103305 A1 US2009103305 A1 US 2009103305A1
Authority
US
United States
Prior art keywords
lamp
pressure gas
gas discharge
lamp bulb
discharge lamp
Prior art date
Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
Abandoned
Application number
US10/596,808
Other languages
English (en)
Inventor
Arnd Ritz
Current Assignee (The listed assignees may be inaccurate. Google has not performed a legal analysis and makes no representation or warranty as to the accuracy of the list.)
Koninklijke Philips NV
Original Assignee
Koninklijke Philips Electronics NV
Priority date (The priority date is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the date listed.)
Filing date
Publication date
Application filed by Koninklijke Philips Electronics NV filed Critical Koninklijke Philips Electronics NV
Assigned to KONINKLIJKE PHILIPS ELECTRONICS N.V. reassignment KONINKLIJKE PHILIPS ELECTRONICS N.V. ASSIGNMENT OF ASSIGNORS INTEREST (SEE DOCUMENT FOR DETAILS). Assignors: RITZ, ARND
Publication of US20090103305A1 publication Critical patent/US20090103305A1/en
Abandoned legal-status Critical Current

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Classifications

    • H—ELECTRICITY
    • H01—ELECTRIC ELEMENTS
    • H01J—ELECTRIC DISCHARGE TUBES OR DISCHARGE LAMPS
    • H01J61/00—Gas-discharge or vapour-discharge lamps
    • H01J61/02—Details
    • H01J61/30—Vessels; Containers
    • H01J61/35—Vessels; Containers provided with coatings on the walls thereof; Selection of materials for the coatings
    • H—ELECTRICITY
    • H01—ELECTRIC ELEMENTS
    • H01J—ELECTRIC DISCHARGE TUBES OR DISCHARGE LAMPS
    • H01J61/00—Gas-discharge or vapour-discharge lamps
    • H01J61/02—Details
    • H—ELECTRICITY
    • H01—ELECTRIC ELEMENTS
    • H01J—ELECTRIC DISCHARGE TUBES OR DISCHARGE LAMPS
    • H01J61/00—Gas-discharge or vapour-discharge lamps
    • H01J61/02—Details
    • H01J61/04—Electrodes; Screens; Shields
    • H01J61/045—Thermic screens or reflectors
    • H—ELECTRICITY
    • H01—ELECTRIC ELEMENTS
    • H01J—ELECTRIC DISCHARGE TUBES OR DISCHARGE LAMPS
    • H01J61/00—Gas-discharge or vapour-discharge lamps
    • H01J61/02—Details
    • H01J61/52—Cooling arrangements; Heating arrangements; Means for circulating gas or vapour within the discharge space

Definitions

  • the invention relates to a high-pressure gas discharge lamp which comprises at least a lamp bulb which hermetically seals off a gas-filled discharge space, which lamp bulb has at least one region which does not and/or does not directly serve for the desired light emission of the high-pressure gas discharge lamp.
  • Regions of the lamp bulb which do not serve directly for the desired light emission of the high-pressure gas discharge lamp may be, for example, coatings or reflectorized portions. These are often made impermeable or partly impermeable at least to visible light or a portion thereof. If this region, for example, reflects light into the lamp bulb, it may serve indirectly for providing the desired light emission.
  • Regions of the lamp bulb which do not primarily serve for the desired light emission of the high-pressure gas discharge lamp may fulfill other functions of the lamp which achieve, for example, also a reduction in the quantity of light but improve lamp life, or the like.
  • the outer surface of the lamp bulb has a region which directly serves for the desired light emission of the high-pressure gas discharge lamp, for example in the form of a light emission window.
  • High-pressure gas discharge lamps (HID or high intensity discharge lamps) and in particular UHP or ultra high performance lamps are preferred for use inter alia in projection applications because of their optical properties.
  • a light source which is point-shaped as much as possible is required for these applications, so that the discharge arc arising between the electrode tips should not exceed a length of approximately 0.5 to 2.5 mm. Furthermore, a luminous intensity which is as high as possible in combination with as natural as possible a spectral composition of the light is usually desired.
  • the highest temperature at the inner surface of the discharge space must not become so high that a devitrification of the lamp bulb occurs, the latter usually being made of quartz glass. This may constitute a problem because the strong convection inside the discharge space of the lamp heats the region above the discharge arc particularly strongly. There is accordingly an inhomogeneous temperature distribution in the discharge space at least during the gas discharge and immediately afterwards.
  • the coldest spot on the inner surface of the lamp bulb in the region of the discharge space must still have such a high temperature, for example approximately1200 K, that a mercury pressure of approximately 200 bar can be achieved, such that the mercury will not deposit there but remains overall in the evaporated state to a sufficient degree. This is to be heeded in particular in lamps with saturated gas fillings.
  • This difference for example, often has values around approximately 120 K in UHP lamps with a reflecting partial coating on the lamp bulb in accordance with the teachings of DE 101 51 267 A1.
  • the highest and the lowest temperature are mutually dependent, in particular in small, highly loaded discharge lamps, and may lead to problems in the adjustment of an optimum lamp operation with a sufficiently long lamp life in certain applications.
  • the discharge space must be so small that a sufficient amount of energy reaches the coldest spot, particular owing to heat conduction, so as to keep the relevant minimum temperature of the coldest spot on the inner surface of the discharge space high enough.
  • UHP lamps usually keep within the required temperature ranges of approximately 1200 K to approximately 1400 K when operated at rated power. It is desirable, however, to widen the possible field of application, for example to achieve a dimming possibility of the lamp or to upgrade a lamp type for applications with a higher lumen output.
  • dimming the temperature of the coldest spot must not drop below the minimum temperature.
  • the temperature of the hottest spot must not exceed the maximum temperature. It is apparent from the above interrelationships that the design of the UHP lamp can be simplified and that the field of application can be widened if suitable measures can be taken to reduce the temperature difference between the coldest and the hottest spot.
  • the object of the invention accordingly is to provide a high-pressure gas discharge lamp of the kind mentioned in the opening paragraph which has a smaller temperature difference between the hottest and the coldest spot, such that these two temperature values lie within the required temperature region between the minimum and the maximum temperature.
  • the relevant solution is to be technically simple and feasible for industrial mass production.
  • the object of the invention is achieved by means of a high-pressure gas discharge lamp which comprises at least a lamp bulb which hermetically seals off a gas-filled discharge space, which lamp bulb has at least one region which does not and/or does not directly serve for the desired light emission of the high-pressure gas discharge lamp, wherein a thermally conducting material is provided which has a higher thermal conductivity than the material of the lamp bulb.
  • the provision according to the invention of the thermally conducting material which has a higher thermal conductivity than the material of the lamp bulb, achieves at least a partial temperature equalization in the region of the outer surface of the lamp bulb in particular owing to the thermal conduction in the thermally conducting material.
  • This temperature equalization in particular achieves a reduction in the higher temperatures and an increase in the lower temperatures preferentially in that region of the lamp bulb which is directly influenced by the corresponding region of the thermally conducting material.
  • the temperature conditions of the other regions of the lamp bulb are influenced at least indirectly, in particular owing to the effects of the thermal conduction in the lamp bulb. The result is a reduction of the temperature difference between the highest and the lowest temperature.
  • the influence on this temperature difference according to the invention i.e. the reduction in this temperature difference, depends inter alia on the relevant lamp type, on the size and arrangement of the region or regions of the thermally conducting material, and on the thermal conduction coefficient of the thermally conducting material.
  • the degree of the influence is accordingly different for different cases, for example this degree increases with an increasing size of the thermally conducting material.
  • the design of the relevant high-pressure discharge lamp may be simplified and/or the relevant operating range may be widened in dependence on the degree of this influence on the temperature difference.
  • the dependent claims 2 to 7 relate to advantageous further embodiments of the high-pressure discharge lamp according to the invention.
  • the high-pressure discharge lamp is a UHP lamp.
  • the discharge space in this lamp type is filled with a quantity of mercury, such that a mercury vapor pressure of, for example, above 200 bar is generated in the discharge space in the case of full evaporation.
  • This high pressure is necessary here for achieving the satisfactory luminous intensity and spectral distribution of the UHP lamp.
  • This vapor pressure can only be maintained above a certain temperature of approximately 1200 K along the entire inner wall of the discharge vessel. When the inner temperature undershoots the required minimum temperature in a location, mercury will condense in this location, so that the pressure drops and the lamp data deteriorate.
  • a part of the energy converted in the discharge arc of the lamp reaches the surface of the discharge chamber and subsequently the surface of the lamp bulb, inter alia owing to convection of the hot gas.
  • the discharge vessel must be comparatively small. The maximum temperature of approximately 1400 K must not be exceeded in the hottest spot, because otherwise the useful life of the lamp would be reduced owing to recrystallization of the lamp bulb.
  • the thermally conducting material is shaped as a sleeve and is arranged at a distance from the lamp bulb of less than approximately 500 ⁇ m, more preferably at a distance of less than approximately 200 ⁇ m.
  • This arrangement is particularly suitable for mass manufacture.
  • metal sleeves may be inexpensively manufactured beforehand and mounted without increased requirements as regards the observance of usual manufacturing tolerances. Given small gap widths between the sleeve and the lamp bulb, however, a sufficient heat transmission, in particular by heat conduction and heat radiation, is still safeguarded.
  • the thermally conducting material is a foil or a coating arranged on the lamp bulb.
  • the choice of material for use as the thermally conducting material particularly favors aluminum and/or copper because of their comparatively good thermal conductivity and availability.
  • the relative thermal conduction coefficients with respect to the value of the thermal conduction coefficient of silver, silver being a very good thermal conductor are, for example: copper approximately 0.95, aluminum approximately 0.585, and glass approximately 0.002.
  • the mutually corresponding surfaces of the lamp bulb and the thermally conducting material are identical or similar to a high degree as regards shape, geometry, and expansion.
  • the desired heat transmission between the mutually corresponding regions of the lamp bulb and of the thermally conducting material can thus be realized particularly effectively.
  • the mutually corresponding surfaces of the lamp bulb and of the thermally conducting material are not or only partly identical or similar as regards shape, geometry, and/or expansion.
  • a suitable choice of these parameters of the thermally conducting material renders it possible, for example, to exert an additional influence on the temperature field, in particular in envisaged points or regions of the lamp bulb. These regions may be so cold in certain applications, for example where the electrodes enter the lamp bulb at the ends thereof, that a condensation effect or temperature stresses arise here.
  • a suitable dimensioning of the thermally conducting material so as to serve as heat bridges provides a heat conduction towards these cold regions via said bridges.
  • the object of the invention is also achieved by means of a lighting unit which comprises at least one high-pressure gas discharge lamp as claimed in any one of the claims 1 to 7 as a light source.
  • the dependent claim 9 relates to advantageous further developments of the lighting unit according to the invention.
  • a lighting unit in accordance with the teachings of DE 101 51 267 A1 is preferred, in which a UHP lamp is used as the light source and the back reflector is arranged on the lamp bulb.
  • This lighting unit achieves an increased efficiency in optical projection systems in particular owing to the reflectorization of part of the surface of the spherical discharge vessel.
  • the object here is to allow as little visible light as possible to issue from the reflectorized portion of the bulb surface.
  • Surface regions not covered by the back reflector serve in particular as light emission windows.
  • the back reflector thus serves for the desired light emission of the high-pressure gas discharge lamp in an indirect manner and is arranged on the surface of a portion of the lamp bulb.
  • the geometrical shape of the back reflector which is dependent on its function, provides particularly favorable design possibilities as regards thermal conduction for the arrangement of the relevant thermally conducting material.
  • FIG. 1 diagrammatically shows a high-pressure gas discharge lamp (UHP lamp) in longitudinal sectional view
  • FIG. 2 shows measured values of a UHP lamp with and without sleeve.
  • FIG. 1 diagrammatically shows a high-pressure gas discharge lamp (UHP lamp) in longitudinal sectional view.
  • a lamp bulb 2 has a discharge space 21 in which a usual discharge gas and an electrode arrangement are present.
  • the electrode arrangement is formed by two electrodes 22 , 23 , between whose tips the gas discharge takes place in a known manner.
  • the lamp bulb 2 and the main reflector 1 are mutually arranged such that the location of the actual light source, i.e. the region between the two electrodes 22 , 23 , lies substantially in the focus of the main reflector 1 .
  • a back reflector 3 in the form of a reflecting layer is present on the substantially spherical portion of the lamp bulb 2 , which has an external diameter of approximately 9 mm.
  • the layer structure and the corresponding material selections may be found, for example, in DE 101 51 267 A1.
  • This portion of the surface is shaped such that light emitted from the gas discharge and incident on the back reflector 3 is reflected through the opening 4 onto the main reflector 1 .
  • the back reflector 3 is usually dimensioned such that it extends not quite up to halfway the region of the lamp bulb 2 surrounding the discharge space 21 .
  • the thermally conducting material in the form of a sleeve 5 is arranged adjacent the back reflector 3 substantially without mechanical contact thereto.
  • the sleeve 5 in particular made of copper, is fastened to the UHP lamp in a usual manner, for example by means of an ignition antenna (not shown in FIG. 1 ) usual for this application.
  • the sleeve 5 is arranged at a distance of less than approximately 200 ⁇ m from the lamp bulb 2 , which renders possible a technically simple mounting and yet a good thermal transmission.
  • the sleeve 5 therefore has a shape corresponding to the substantially spherical region of the lamp bulb 2 in this region.
  • the dimensions of the sleeve 5 are chosen such that no additional shadow effect is caused in the light coming from the back reflector 3 . Since the region below the sleeve 5 is reflectorized, little or no light reaches the surface of the sleeve 5 , so that the optical properties of the lamp are not affected thereby.
  • the high thermal conductivity of the sleeve 5 has the result that temperature gradients across the sleeve 5 are small in comparison with the temperature difference across the lamp bulb 2 .
  • the regions of the sleeve 5 close to the hottest and to the coldest spot of the adjoining lamp bulb 2 are substantially at one temperature level.
  • the temperature gradients present between the sleeve 5 and the surface of the lamp bulb 2 achieve overall an energy flow from the hot to the cold regions of the lamp bulb 2 .
  • FIG. 2 shows the temperature gradient without a sleeve (dotted line) and with a sleeve (block line) in a diagram.
  • the location of the temperature profile recorded from top to bottom is plotted from left to right on the X-axis, with the UHP lamp in horizontal position, i.e. the electrodes 22 , 23 are on a horizontal axis.
  • the temperature values in ° C. are plotted on the Y-axis.
  • the temperature registration (dotted line) without sleeve results in a temperature difference of approximately 124 K, with the hottest spot determined at approximately 907° C. and the coldest spot at approximately 783° C.
  • the temperature registration (block line) with sleeve 5 yields a temperature difference of approximately 70 K, with the hottest spot determined at approximately 887° C. and the coldest sot at approximately 817° C.

Landscapes

  • Vessels And Coating Films For Discharge Lamps (AREA)
  • Discharge Lamps And Accessories Thereof (AREA)
  • Non-Portable Lighting Devices Or Systems Thereof (AREA)
  • Gas Separation By Absorption (AREA)
  • Securing Globes, Refractors, Reflectors Or The Like (AREA)
  • Arrangement Of Elements, Cooling, Sealing, Or The Like Of Lighting Devices (AREA)
US10/596,808 2004-01-06 2004-12-21 High-pressure gas discharge lamp Abandoned US20090103305A1 (en)

Applications Claiming Priority (3)

Application Number Priority Date Filing Date Title
EP04100010.0 2004-01-06
EP04100010 2004-01-06
PCT/IB2004/052876 WO2005076312A2 (fr) 2004-01-06 2004-12-21 Lampe a decharge dans un gaz a haute pression

Publications (1)

Publication Number Publication Date
US20090103305A1 true US20090103305A1 (en) 2009-04-23

Family

ID=34833699

Family Applications (1)

Application Number Title Priority Date Filing Date
US10/596,808 Abandoned US20090103305A1 (en) 2004-01-06 2004-12-21 High-pressure gas discharge lamp

Country Status (8)

Country Link
US (1) US20090103305A1 (fr)
EP (1) EP1704581B1 (fr)
JP (1) JP2007518225A (fr)
CN (1) CN1902730A (fr)
AT (1) ATE422098T1 (fr)
DE (1) DE602004019303D1 (fr)
TW (1) TW200527477A (fr)
WO (1) WO2005076312A2 (fr)

Cited By (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US20080170308A1 (en) * 2007-01-12 2008-07-17 Asml Netherlands B.V. Cover for shielding a portion of an arc lamp
US20090045745A1 (en) * 2005-12-28 2009-02-19 Shunsuke Kakisaka Illumination device and metal vapor discharge lamp

Citations (5)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US1232046A (en) * 1915-05-22 1917-07-03 Firm Robert Bosch Projection-lamp.
US5479065A (en) * 1992-12-28 1995-12-26 Toshiba Lighting & Technology Corporation Metal halide discharge lamp suitable for an optical light source having a bromine to halogen ratio of 60-90%, a wall load substantially greater than 40 W/cm2, and a D.C. potential between the anode and cathode
US5660462A (en) * 1994-09-13 1997-08-26 Osram Sylvania Inc. High efficiency vehicle headlights and reflector lamps
US6002197A (en) * 1996-04-24 1999-12-14 Ushiodenki Kabushiki Kaisha Metal halide lamp light source device having conducting wire positioned to prevent it from casting a shadow
US6558032B2 (en) * 2000-08-25 2003-05-06 Stanley Electric Co., Ltd. LED lighting equipment for vehicle

Family Cites Families (4)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPH05283051A (ja) * 1992-04-01 1993-10-29 Iwasaki Electric Co Ltd メタルハライドランプ装置
JPH1092385A (ja) * 1996-09-12 1998-04-10 Matsushita Electron Corp 管 球
JP2002151005A (ja) * 2000-11-14 2002-05-24 Ushio Inc 放電ランプ
DE10151267A1 (de) * 2001-10-17 2003-04-30 Philips Corp Intellectual Pty Beleuchtungseinheit

Patent Citations (5)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US1232046A (en) * 1915-05-22 1917-07-03 Firm Robert Bosch Projection-lamp.
US5479065A (en) * 1992-12-28 1995-12-26 Toshiba Lighting & Technology Corporation Metal halide discharge lamp suitable for an optical light source having a bromine to halogen ratio of 60-90%, a wall load substantially greater than 40 W/cm2, and a D.C. potential between the anode and cathode
US5660462A (en) * 1994-09-13 1997-08-26 Osram Sylvania Inc. High efficiency vehicle headlights and reflector lamps
US6002197A (en) * 1996-04-24 1999-12-14 Ushiodenki Kabushiki Kaisha Metal halide lamp light source device having conducting wire positioned to prevent it from casting a shadow
US6558032B2 (en) * 2000-08-25 2003-05-06 Stanley Electric Co., Ltd. LED lighting equipment for vehicle

Cited By (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US20090045745A1 (en) * 2005-12-28 2009-02-19 Shunsuke Kakisaka Illumination device and metal vapor discharge lamp
US8063566B2 (en) * 2005-12-28 2011-11-22 Panasonic Corporation Illumination apparatus and metal vapor discharge lamp
US20080170308A1 (en) * 2007-01-12 2008-07-17 Asml Netherlands B.V. Cover for shielding a portion of an arc lamp

Also Published As

Publication number Publication date
WO2005076312A3 (fr) 2006-03-02
EP1704581A2 (fr) 2006-09-27
TW200527477A (en) 2005-08-16
JP2007518225A (ja) 2007-07-05
EP1704581B1 (fr) 2009-01-28
DE602004019303D1 (de) 2009-03-19
ATE422098T1 (de) 2009-02-15
CN1902730A (zh) 2007-01-24
WO2005076312A2 (fr) 2005-08-18

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Legal Events

Date Code Title Description
AS Assignment

Owner name: KONINKLIJKE PHILIPS ELECTRONICS N.V., NETHERLANDS

Free format text: ASSIGNMENT OF ASSIGNORS INTEREST;ASSIGNOR:RITZ, ARND;REEL/FRAME:021807/0349

Effective date: 20041221

STCB Information on status: application discontinuation

Free format text: ABANDONED -- FAILURE TO RESPOND TO AN OFFICE ACTION

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